WO2004001453A1 - Pulse sequences for exciting nuclear quadrupole resonance - Google Patents
Pulse sequences for exciting nuclear quadrupole resonance Download PDFInfo
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- WO2004001453A1 WO2004001453A1 PCT/AU2003/000777 AU0300777W WO2004001453A1 WO 2004001453 A1 WO2004001453 A1 WO 2004001453A1 AU 0300777 W AU0300777 W AU 0300777W WO 2004001453 A1 WO2004001453 A1 WO 2004001453A1
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- pulse
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- pulse sequences
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Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01R—MEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
- G01R33/00—Arrangements or instruments for measuring magnetic variables
- G01R33/20—Arrangements or instruments for measuring magnetic variables involving magnetic resonance
- G01R33/44—Arrangements or instruments for measuring magnetic variables involving magnetic resonance using nuclear magnetic resonance [NMR]
- G01R33/441—Nuclear Quadrupole Resonance [NQR] Spectroscopy and Imaging
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N24/00—Investigating or analyzing materials by the use of nuclear magnetic resonance, electron paramagnetic resonance or other spin effects
- G01N24/08—Investigating or analyzing materials by the use of nuclear magnetic resonance, electron paramagnetic resonance or other spin effects by using nuclear magnetic resonance
- G01N24/084—Detection of potentially hazardous samples, e.g. toxic samples, explosives, drugs, firearms, weapons
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01R—MEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
- G01R33/00—Arrangements or instruments for measuring magnetic variables
- G01R33/20—Arrangements or instruments for measuring magnetic variables involving magnetic resonance
- G01R33/44—Arrangements or instruments for measuring magnetic variables involving magnetic resonance using nuclear magnetic resonance [NMR]
- G01R33/48—NMR imaging systems
- G01R33/54—Signal processing systems, e.g. using pulse sequences ; Generation or control of pulse sequences; Operator console
- G01R33/56—Image enhancement or correction, e.g. subtraction or averaging techniques, e.g. improvement of signal-to-noise ratio and resolution
- G01R33/561—Image enhancement or correction, e.g. subtraction or averaging techniques, e.g. improvement of signal-to-noise ratio and resolution by reduction of the scanning time, i.e. fast acquiring systems, e.g. using echo-planar pulse sequences
- G01R33/5613—Generating steady state signals, e.g. low flip angle sequences [FLASH]
Definitions
- the present invention relates to the practical use of the nuclear quadrupole resonance (NQR) phenomenon for identifying substances that contain quadrupole nuclei with either integer or half-integer spins, particularly for identifying explosive or narcotic substances.
- NQR nuclear quadrupole resonance
- the invention has particular utility in multi-pulse radio frequency (RF) excitation of quadrupole nuclei and to the subsequent measurement of the NQR signal emitted therefrom where the effect of temperature upon the measurerhent is mitigated.
- RF radio frequency
- purging pulse means both a separate preparatory pulse and a group of preparatory pulses.
- a group of preparatory pulses means a group of pulses that precede a multi-pulse sequence distributed within time interval ⁇ 3T (T lp being the time of spin-lattice relaxation in a rotating coordinate system), during which the NQR signal, as a rule, is not measured.
- the body of the sequence is used to signify a multi-pulse sequence with subtracted preparatory pulses; the measurement of an NQR signal usually occurring when the "body of the sequence” is in action.
- any solid sample containing quadrupole nuclei can be characterised by three parameters: the spin-lattice relaxation time T the spin-spin relaxation time T 2 and the time of the induction signal damping T 2 * .
- multi-pulse sequences can be classified into the following general groups:
- Sequences of single pulses which can include multi-pulse sequences of any type, if intervals between the pulses in these sequences exceed the spin-lattice relaxation time T j .
- All echo-sequences (sequences composed of a certain number of pulses which are organised in such a way that the NQR signal is formed not directly after the radio frequency irradiation pulse, but after a certain delay, necessary for refocussing the magnetic momentum of the sample nuclei) could also be regarded as belonging to this type of sequence, because for the optimal formation of the echo signal the condition T 2 * ⁇ ⁇ ⁇ T 2 should hold true.
- One of the main peculiarities of this type of sequence is its capability to saturate the quadrupolar spin system of the sample.
- Multi-pulse sequences of the Steady State Free Precession (SSFP) type Intervals between pulses in these sequences ( ⁇ ) fulfil the condition of ⁇ ⁇ T 2 * .
- This type can include quite complex formations, containing not only SSFP sequences but also special techniques for destroying the SSFP state; this "destruction" can be achieved by including the magnetic field gradient pulses, by using composite pulses, by forming a special phase alternation of the RF carrier frequency, etc.
- the fifth group does not have any individual physical characteristics that do not relate to at least one of the previous groups. Therefore, only aspects of the first four groups of sequences in the above classification will be considered further.
- Single pulses can only create a free induction decay (FID) signal, entirely determined - as well as magneto-acoustic ringing, piezo-electric effects and the spurious signals of the resonance circuit of the NQR detector probe - by the pulse that generated it.
- FID free induction decay
- Time available for accumulating the NQR signal is limited by the time constant T le ⁇ ;
- echo sequences does not help to detect a number of substances that have a little or zero asymmetry parameter, as the amplitude of echo-signals decreases with the decrease of the asymmetry parameter.
- the stochastic resonance requires lower peak powef.
- the peak power can be tens and even hundreds times lower than when using coherent pulses and still achieve similar sensitivity.
- Stochastic sequences belong to saturating sequences; however the saturation of the spin system limits the time of the NQR signal accumulation, as is the case with Group II sequences, which is equivalent to a loss of sensitivity; it does not produce the advantages that Group II sequences can offer using echo signals.
- ⁇ is the pulse spacing of the sequence
- n and m are whole numbers
- ⁇ eI represents the effective field which substitutes the effect of the RF pulses and the resonance offset.
- the SSFP sequences allow ⁇ achievement of a greater signal-to-noise ratio per unit of time than any other multi- pulse sequences used for exciting the quadrupole spin system.
- the dependence of the signal intensity on the resonance offset when using the SSFP sequences is characterised by the existence of intensity anomalies and these intensity anomalies make the SSFP group sensitive to the changes in the resonance frequency of the quadrupole spin system during temperature changes.
- the first SSFP sequence consisting of identical coherent RF pulses was used in NMR in 1951 and later studied in great detail. In NQR, this sequence was first used for measuring the T t of the 14 N resonance line in hexamethylene tetramine.
- the basic version of the SSFP sequences was used - a sequence of coherent equally spaced pulses with a flip angle ⁇ and the repetition cycle ⁇ : ⁇ l2 - ⁇ - ⁇ l2 , where n is the number of the sequence cycles (it is also possible to write it down as [ ⁇ - ⁇ ).
- the irradiation was done with different series of pulses, with the carrier frequency
- the difference in the frequency of both carrier frequencies corresponds to the difference between the frequencies at which the maximum and the minimum signal intensity was observed.
- the signals received after ⁇ pulses of the NPAPS sequence and after ⁇ _ x pulses of the PAPS sequence are subtracted, and those received after ⁇ of the PAPS sequence are added together. This allows not only a decrease in intensity anomalies, but also elimination of magneto-acoustic ringing.
- the signals received after ⁇ pulses of both PAPS and NPAPS sequences are added up with the positive sign, and after ⁇ x pulses they are added with the negative sign.
- the maximum accumulated signal achieved by using either method of accumulation is less than the maximum achieved when using only NPAPS or
- curves corresponding to two dependencies of NQR signal on the frequency received for NaNO 2 are shown, after irradiation with NPAPS and PAPS sequences using the accumulation rules determined by the first method described above (curve 1 ) and the second method (curve 2), respectively.
- a principal object of the present invention is to increase the accuracy of detection in specimens of prescribed substances such as, but not limited to, certain explosives and narcotics compared with previously known methods of detecting same using NQR.
- the principal object is achieved by using a combination of two or more sequences, arranged so that a definite regularity of the phase alteration of pulses in each of the sequences is equivalent to a shift of spectral components of the sequences in relation to each other, and in at least one of the sequences, not less than two phases are alternating
- At least one of the sequences contains a preparatory pulse.
- an apparatus for producing a multi-pulse sequence of the kind described for irradiating a substance provided with quadrupole nuclei with either integer or half-integer spins to detect an NQR signal emitted therefrom the apparatus having pulse sequence generating means to produce said multi-pulse sequence.
- a method detecting a class of explosive or narcotic substances containing quadrupolar nuclei in a sample using nuclear quadrupole resonance including the following steps:
- the pulse sequences consisting of pulses that contain phases of the carrier frequency chosen from a certain set of unmatched phases distributed within the interval from 0 to 2 ⁇ radian, with every sequence different from the others either by the number of phases chosen from the set, or by the sequence order inside the sequence;
- the method includes detecting nuclear quadrupole resonance signals when the combination of the pulse sequences irradiates the sample; and
- the predetermined frequency of the pulse sequence is near to one of the NQR frequencies of the substances to be detected.
- a combination of two or more sequences different from a combination of PAPS and NPAPS arranged so that a definite regularity of the phase alteration of pulses in each of the sequences is equivalent to a shift of spectral components of the sequences in relation to each other, and in at least one of the sequences not less than two phases are alternating and none of the sequences contains a preparatory pulse.
- a method of detecting a class of explosive or narcotic substances containing quadrupolar nuclei in a sample using nuclear quadrupole resonance including the following steps:
- the pulse sequences consisting of pulses that contain phases of the carrier frequency chosen from a certain set of unmatched phases distributed within the interval from 0 to 2 ⁇ radian, with every sequence different from the others either by the number of phases chosen from the set, or by the sequence order inside the sequence;
- the method includes detecting nuclear quadrupole resonance signals when the combination of the pulse sequences irradiates the sample; and combining all said nuclear quadrupole resonance signals to generate the resulting signal.
- the principal object of the invention is achieved by completing one measurement act using a combination that consists of at least two multi-pulse sequences having the same carrier frequency of the RF pulses, but different phase shifts between pulses in each sequence of the said combination.
- any spin system has a non-zero "phase memory” time.
- phase memory manifests itself in the fact that a sudden momentary perturbation of the spin system influences its evolution for a certain period of time. This phenomenon can be used to change the dependence of the NQR signal on the frequency offset to reduce the effect of temperature.
- preparatory pulses or groups of preparatory pulses may be used that are switched on before one or several sequences of the combination.
- the rules of addition are determined by the first method (curve 1) and the second method (curve 2) respectively, as described in the aforementioned discussion of background art;
- FIG.2 is a graph similar to Fig 1, but demonstrating examples of the effect of preparatory pulses on the value of the NQR signal in accordance with the first embodiment, where the preparatory pulses are switched on before the PAPS sequence:
- FIG.3 is another graph, similar to Figs 1 and 2, but showing an example of using PAPS and NPAPS sequences in accordance with the first embodiment with preparatory pulses at the frequency v_ for NaNO 2 , wherein:
- Curve 1 corresponds to PAPS and NPAPS sequences with preparatory pulses:
- curve 2 is the result of an experiment with these sequences with the same number of accumulations but without preparatory pulses, corresponding to the second method described in relation to the background art;
- FIG.5 is a graph similar to those of the preceding figures, but showing two examples of using a combination of sequences without preparatory pulses in accordance with the second embodiment, the sequences being:
- the best mode for carrying out the invention is concerned with using multi-pulse RF sequences to excite an NQR signal in a substance containing quadrupole nuclei with either integer or half-integer spins for the purposes of detecting such a signal.
- the particular apparatus for producing pulse sequences of this kind comprises a pulse generator, the hardware design of which is known, and described in the applicant's corresponding International Patent Application PCT/AU00/01214 (WO 01/25809), which is incorporated herein by reference.
- the particular apparatus for producing pulse sequences of this kind comprises a pulse generator, the hardware design of which is known, and described in the applicant's corresponding International Patent Application PCT/AU00/01214 (WO 01/25809), which is incorporated herein by reference.
- a pulse programmer is used to create a low voltage level pulse sequence.
- Such programmer is capable of generating a continuous sine wave of a desired frequency (eg; 0.89 or 5.2MHz) and of any phase by using a Direct Digital Synthesizer (DDS) or any RF source.
- DDS Direct Digital Synthesizer
- a gate is used to divide the continuous sine wave into small pulses.
- the gate switches on for ⁇ 300 ⁇ s and off for ⁇ 300 ⁇ s, repeatedly thereby creating a sequence of pulses.
- the user of the pulse generator generates the pulse sequence via a computer program in the controlling computer.
- the computer program enables the user to input the frequency, phase, duration and separation of any pulses and allows the user to repeat any parts of the pulse sequence in a loop.
- the entire pulse sequence is contained in the program and then converted into binary and sent to the pulse programmer and stored in memory.
- the CPU of the pulse programmer then takes the machine code stored in memory and creates the pulse sequence by changing the frequency and phase of the DDS and providing instructions to the gate as to when to switch, thereby creating the pulses.
- each pulse sequence is transmitted to the coil via a high power amplifier (1 ⁇ 5kW), which amplifies the low voltage signal created by the pulse programmer to a higher voltage level which is sufficient to stimulate the nitrogen 14 nuclei.
- temperature effects on the ability to detect and measure the NQR signal may be reduced by using multiple pulse sequences in which "the bodies of sequences" contain RF pulses with various sets of the carrier frequency phases.
- the best mode for carrying out the invention involves producing a combination of two or more pulse sequences, arranged so that a definite regularity of the phase alteration of RF pulses in each of the pulse sequences occurs, which is equivalent to a shift of the spectral components of the pulse sequences in relation to each other, and further, in at least one of the pulse sequences, there are not less than two phases alternating.
- the body of each pulse sequence must contain pulse cycles (at least one), with the pulses of each cycle containing one of the following N! sets of the carrier frequency phases:
- one set of phases being of the type: ⁇ l 2 , .... .... ⁇ l ⁇ ;
- N sets of phases being of the type: ⁇ 2 ⁇ , ⁇ 2 2 , .... ⁇ 2., .... 2 ⁇ _ ⁇ ;
- N sets of phases being of the type: ⁇ ' N l .
- the set is equivalent to the set ⁇ k . If the bodies of all sequences used in one detection process for a sample contain the same set of phases, they must differ from each other by at least the order of alternation of the pulse phases.
- One embodiment of the best mode for carrying out the present invention is concerned with improving the detection of substances having a relaxation time T t comparable with the time of the duration of the pulse sequence.
- a preparatory pulse is used in an SSFP sequence to improve the value of the NQR signal.
- a preparatory pulse included in an SSFP sequence the characteristics of this type of sequence will now be considered in detail.
- transient processes decay at times t ⁇ 3T 2 , and are replaced by a quasi-stationary state.
- T lp is the time of spin- lattice relaxation in the rotating frame
- the spin-system completely adopts the stationary state and on meeting the condition of n - ⁇ ejr ⁇ m -— a different from ⁇ zero NQR signal exists as long as it is needed.
- phase memory of the spin system is limited by the time interval being ⁇ 3T , means that a "group of preparatory pulses" may be provided, as well as a single preparatory pulse.
- the first specific embodiment of the best mode for carrying out the present invention involves producing the multi-pulse sequence of the best mode in an SSFP type sequence, including a "preparatory pulse” or a" group of preparatory pulses" in at least one of the pulse sequences and the use of the quasi-stationary state in the pulse sequence to "remember” the effect of the preparatory pulse.
- the preparatory pulse increases the intensity of the NQR signal and at the same time reduces the temperature effects in the detection of a prescribed substance containing quadrupole nuclei in a specimen of such.
- FIG.2 shows examples of the influence of preparatory pulses, used prior to the PAPS seq 1 uence ⁇ n Q ⁇ - - t de ,lay - T acq ,(+x) - ⁇ ' -x - t delay - T acq(-x) J n , 7 up * on the value of the NQR signal detected in experiments carried out on a sample of NaNO 2 on line v . In all cases the experiments were carried out at room temperature.
- the duration of the multi-pulse sequence in these examples is less than the spin- lattice relaxation time T r
- ⁇ p 0 is the flip angle of the preparatory pulse
- ⁇ p is the flip angle of the pulses of the sequence body
- ⁇ is the phase of the preparatory pulse
- t dclay is the time of the delay exceeding the "dead time" of the receiver system
- T ⁇ is acquisition time
- ⁇ is the receiver phase.
- curve 2 was received without the preparatory pulse
- Figures 3 and 4 show two examples of the use of the first embodiment.
- the magnetic field component B, of the RF pulses was 4.5 Gauss.
- the duration of the 90° pulse in the powder sample was 68 ⁇ s .
- Figure 3 shows an example of using PAPS and NPAPS sequences with spin- lattice relaxation preparatory pulses.
- Curve 1 corresponds to the PAPS and NPAPS sequences with spin-lattice relaxation preparatory pulses
- curve 2 shows experimental results for the same sequences with the same number of accumulations but without the spin-lattice relaxation preparatory pulses (as in the second method described previously with respect to the background art).
- the duration of each sequence was less than 170 ms, and the interval between the sequences was 2 s.
- the use of spin-lattice relaxation preparatory pulses does not allow an increase in the intensity of the NQR signal at the minimum points, but beyond the narrow areas, near the minimum, the signal intensity is considerably increased.
- FIG.4 shows the result of using four sequences for detecting powdered RDX, the sequences being of the following type:
- the duration of delays, pulses and acquisition times coincides completely with the previous example.
- the intervals between sequences are also 2 s.
- the second embodiment for carrying out the invention achieves a reduction in temperature effects by using a combination of two or more sequences other than PAPS and NPAPS, arranged so that a definite regularity of phase alternation of RF pulses in each of the sequences is equivalent to a shift of the spectrum components of the sequences in relation to each other.
- At least one of the sequences contains not less than two alternating phases and no sequences are arranged so that a definite regularity of the phase alteration of RF pulses in each of the sequences is equivalent to a shift of spectral components of the sequences in relation to each other.
- This embodiment is intended for detecting substances with a relaxation time T, much shorter than the duration of the pulse sequence T .
- sequences For reducing temperature effects the sequences must contain pulses with various sets of the carrier frequency phases.
- phase of the first pulse of each sequence is taken to be zero irrespective of its actual value.
- the phases of all pulses of each sequence will be determined in relation to the phase of the first pulse of this sequence.
- each pulse sequence must contain cycles of pulses (at least one), with the pulses of each cycle containing one of the following N! sets of carrier frequency phases:
- N sets of phases of the following type: ⁇ 2 x , ⁇ 2 2 , .... ⁇ 2., .... J2 Ni ;
- Set is equivalent to set ⁇ k .
- sequences from one combination used in one detection process contain the same pulse phase set, they must differ by at least the sequence order of the phase alternation.
- the magnetic field component B, of the RF pulses equalled 4.5 Gauss.
- Curve 2 corresponds to the combination of the same sequences but in the second sequence the phase of the receiver is changed to the opposite:
- the interval between sequences is two seconds.
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Priority Applications (3)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
AU2003240293A AU2003240293A1 (en) | 2002-06-20 | 2003-06-20 | Pulse sequences for exciting nuclear quadrupole resonance |
US10/518,480 US7355400B2 (en) | 2002-06-20 | 2003-06-20 | Pulse sequences for exciting nuclear quadrupole resonance |
EP03729708A EP1535087A4 (en) | 2002-06-20 | 2003-06-20 | Pulse sequences for exciting nuclear quadrupole resonance |
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AUPS3077 | 2002-06-20 | ||
AUPS3077A AUPS307702A0 (en) | 2002-06-20 | 2002-06-20 | Pulse sequences for exciting nuclear quadrupole resonance |
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WO2004001453A1 true WO2004001453A1 (en) | 2003-12-31 |
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PCT/AU2003/000777 WO2004001453A1 (en) | 2002-06-20 | 2003-06-20 | Pulse sequences for exciting nuclear quadrupole resonance |
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US (1) | US7355400B2 (en) |
EP (1) | EP1535087A4 (en) |
AU (1) | AUPS307702A0 (en) |
WO (1) | WO2004001453A1 (en) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
EP1540380A1 (en) * | 2002-06-21 | 2005-06-15 | QR Sciences Ltd | Pulse sequences for exciting nuclear quadrupole resonance |
WO2015097381A1 (en) | 2013-12-23 | 2015-07-02 | L'air Liquide, Societe Anonyme Pour L'etude Et L'exploitation Des Procedes Georges Claude | Process for the manufacture of glass elements |
Families Citing this family (4)
Publication number | Priority date | Publication date | Assignee | Title |
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WO2012173635A1 (en) * | 2011-06-13 | 2012-12-20 | Vanderbilt University | Multiple resonance nmr spectroscopy using a single transmitter |
US10338015B2 (en) * | 2013-03-04 | 2019-07-02 | The Regents Of The University Of California | Methods and apparatus for analysis of sealed containers |
US11543477B2 (en) * | 2019-04-16 | 2023-01-03 | Vadum, Inc. | Magnetic resonance detection (MRD) system for and methods of detecting and classifying multiple chemical substances |
CN114070679B (en) * | 2021-10-25 | 2023-05-23 | 中国电子科技集团公司第二十九研究所 | Pulse intelligent classification-oriented frequency-phase characteristic analysis method |
Citations (3)
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GB2200462A (en) * | 1987-01-27 | 1988-08-03 | Nat Res Dev | Methods and apparatus for detecting certain compounds |
US5365171A (en) * | 1992-11-30 | 1994-11-15 | The United States Of America As Represented By The Secretary Of The Navy | Removing the effects of acoustic ringing and reducing temperature effects in the detection of explosives by NQR |
WO1996026453A2 (en) * | 1995-02-24 | 1996-08-29 | British Technology Group Limited | Method of and apparatus for nuclear quadrupole resonance testing a sample, and pulse sequence for exciting nuclear quadrupole resonance |
Family Cites Families (10)
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GB2255830B (en) | 1991-04-02 | 1995-03-08 | British Tech Group | Method of and apparatus for NQR testing |
GB9109592D0 (en) | 1991-05-02 | 1991-07-17 | Nat Res Dev | Methods and apparatus for detecting substances |
US5233300A (en) | 1991-05-23 | 1993-08-03 | The United States Of America As Represented By The Secretary Of The Navy | Detection of explosive and narcotics by low power large sample volume nuclear quadrupole resonance (NQR) |
GB9125883D0 (en) | 1991-12-05 | 1992-02-05 | Nat Res Dev | Improvements in nqr testing |
US5592083A (en) * | 1995-03-08 | 1997-01-07 | Quantum Magnetics, Inc. | System and method for contraband detection using nuclear quadrupole resonance including a sheet coil and RF shielding via waveguide below cutoff |
US5608321A (en) | 1995-12-28 | 1997-03-04 | The United States Of America As Represented By The Secretary Of The Navy | Method and apparatus for detecting target species having quadropolar muclei by stochastic nuclear quadrupole resonance |
GB9721892D0 (en) | 1997-10-15 | 1997-12-17 | British Tech Group | Apparatus for and method of testing a sample |
US6577128B1 (en) | 1998-10-15 | 2003-06-10 | Btg International Limited | NQR method and apparatus for testing a sample by applying multiple excitation blocks with different delay times |
US6392408B1 (en) | 1998-05-06 | 2002-05-21 | Quamtum Magnetics, Inc. | Method and system for cancellation of extraneous signals in nuclear quadrupole resonance spectroscopy |
US6307368B1 (en) * | 1999-05-14 | 2001-10-23 | Board Of Trustees Of The Leland Stanford Junior University | Linear combination steady-state free precession MRI |
-
2002
- 2002-06-20 AU AUPS3077A patent/AUPS307702A0/en not_active Abandoned
-
2003
- 2003-06-20 US US10/518,480 patent/US7355400B2/en not_active Expired - Fee Related
- 2003-06-20 WO PCT/AU2003/000777 patent/WO2004001453A1/en not_active Application Discontinuation
- 2003-06-20 EP EP03729708A patent/EP1535087A4/en not_active Withdrawn
Patent Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
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GB2200462A (en) * | 1987-01-27 | 1988-08-03 | Nat Res Dev | Methods and apparatus for detecting certain compounds |
US5365171A (en) * | 1992-11-30 | 1994-11-15 | The United States Of America As Represented By The Secretary Of The Navy | Removing the effects of acoustic ringing and reducing temperature effects in the detection of explosives by NQR |
WO1996026453A2 (en) * | 1995-02-24 | 1996-08-29 | British Technology Group Limited | Method of and apparatus for nuclear quadrupole resonance testing a sample, and pulse sequence for exciting nuclear quadrupole resonance |
Non-Patent Citations (1)
Title |
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See also references of EP1535087A4 * |
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
EP1540380A1 (en) * | 2002-06-21 | 2005-06-15 | QR Sciences Ltd | Pulse sequences for exciting nuclear quadrupole resonance |
EP1540380A4 (en) * | 2002-06-21 | 2007-09-19 | Qr Sciences Ltd | Pulse sequences for exciting nuclear quadrupole resonance |
WO2015097381A1 (en) | 2013-12-23 | 2015-07-02 | L'air Liquide, Societe Anonyme Pour L'etude Et L'exploitation Des Procedes Georges Claude | Process for the manufacture of glass elements |
Also Published As
Publication number | Publication date |
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EP1535087A4 (en) | 2006-05-24 |
AUPS307702A0 (en) | 2002-07-11 |
US20060091883A1 (en) | 2006-05-04 |
EP1535087A1 (en) | 2005-06-01 |
US7355400B2 (en) | 2008-04-08 |
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